Take free online mock test for National Institute of Open Schooling (NIOS) Class XII Physics (312) chapter 'Kinetic Theory of Gases'. 20 MCQs, 20 minutes, detailed solutions & score analysis.
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Mastering Kinetic Theory of Gases in Class 12 provides critical subject intuition, analytical skills, and examination readiness.
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| Term / Formula | Type | Definition / Meaning | Explanation / Notes | Example / Usage |
|---|---|---|---|---|
| Core Concept | Principle | Primary concept governing Kinetic Theory of Gases. | मुख्य सिद्धांत | "Understand and apply the principle accurately." |
| Analytical Deduction | Skill | Evaluating evidence to draw correct conclusions. | तार्किक विश्लेषण | "Examine question clues systematically." |
Here is a sneak peek of the questions included in this test set. Test your preparation by viewing the answer and detailed explanation before starting the timed exam.
In the microscopic derivation of gas pressure for $N$ identical molecules of mass $m$ in a cubic box of side $L$ (shown below):
A molecule with velocity component $v_x$ undergoes elastic collisions with the perpendicular face of area $L^2$. Considering all molecules with isotropic velocity distribution $\overline{v_x^2} = \frac{1}{3} v_{\text{rms}}^2$, the pressure exerted on the face is:
पक्ष के एक घन बॉक्स में $N$ द्रव्यमान के समान अणुओं $m$ के लिए गैस के दबाव की सूक्ष्म व्युत्पत्ति में $L$ (नीचे दिखाया गया है):
[[एच0एच]]वेग घटक वाला एक अणु $v_x$ क्षेत्र के लंबवत चेहरे के साथ लोचदार टकराव से गुजरता है $L^2$। आइसोट्रोपिक वेग वितरण वाले सभी अणुओं को ध्यान में रखते हुए $\overline{v_x^2} = \frac{1}{3} v_{\text{rms}}^2$, चेहरे पर लगाया गया दबाव है:
$P = \frac{1}{3}\rho v_{\text{rms}}^2$
$P = \frac{1}{2}\rho v_{\text{rms}}^2$
$P = \rho v_{\text{rms}}^2$
$P = \frac{2}{3}\rho v_{\text{rms}}^2$
Step-by-step solution:
1. In each elastic collision with the wall at $x = L$, momentum change is $\Delta p_x = 2 m v_x$.
2. The time between successive collisions of this molecule with the same wall is $\Delta t = \frac{2L}{v_x}$.
3. Average force contributed by this molecule: $F_i = \frac{\Delta p_x}{\Delta t} = \frac{m v_{xi}^2}{L}$.
4. Total force on the wall of area $A = L^2$:
$$F_{\text{total}} = \sum_{i=1}^N \frac{m v_{xi}^2}{L} = \frac{m}{L} N \overline{v_x^2}$$
5. By isotropy, $\overline{v_x^2} = \frac{1}{3} v_{\text{rms}}^2$, and volume is $V = L^3$:
$$P = \frac{F_{\text{total}}}{L^2} = \frac{N m}{L^3} \left(\frac{1}{3} v_{\text{rms}}^2\right) = \frac{1}{3}\rho v_{\text{rms}}^2$$
चरण-दर-चरण समाधान:
1. $x = L$ पर दीवार के साथ प्रत्येक लोचदार टकराव में, गति परिवर्तन $\Delta p_x = 2 m v_x$ होता है।
2. एक ही दीवार से इस अणु के क्रमिक टकराव के बीच का समय $\Delta t = \frac{2L}{v_x}$ है।
3. इस अणु द्वारा योगदान किया गया औसत बल: $F_i = \frac{\Delta p_x}{\Delta t} = \frac{m v_{xi}^2}{L}$।
4. क्षेत्र की दीवार पर कुल बल $A = L^2$:
$$F_{\text{total}} = \sum_{i=1}^N \frac{m v_{xi}^2}{L} = \frac{m}{L} N \overline{v_x^2}$$
5. आइसोट्रॉपी द्वारा, $\overline{v_x^2} = \frac{1}{3} v_{\text{rms}}^2$, और आयतन है $V = L^3$:
$$P = \frac{F_{\text{total}}}{L^2} = \frac{N m}{L^3} \left(\frac{1}{3} v_{\text{rms}}^2\right) = \frac{1}{3}\rho v_{\text{rms}}^2$$
A chamber containing Helium ($\text{He}$, $M_1 = 4.0\text{ g/mol}$) and another containing an unknown hydrocarbon gas are set up at identical temperature and pressure, as depicted below:
Helium effuses through the pinhole into the vacuum at a rate that is $4.0\text{ times}$ faster than the unknown hydrocarbon. The molar mass $M_{\text{unknown}}$ of the hydrocarbon is:
एक कक्ष जिसमें हीलियम ($\text{He}$, $M_1 = 4.0\text{ g/mol}$ ) और एक अन्य कक्ष जिसमें अज्ञात हाइड्रोकार्बन गैस है, समान तापमान और दबाव पर स्थापित किए गए हैं, जैसा कि नीचे दर्शाया गया है:
[[एच0एच]]हीलियम पिनहोल के माध्यम से निर्वात में उस दर से प्रवाहित होता है जो अज्ञात हाइड्रोकार्बन की तुलना में $4.0\text{ times}$ तेज है। हाइड्रोकार्बन का दाढ़ द्रव्यमान $M_{\text{unknown}}$ है:
$16.0\text{ g/mol}$
$64.0\text{ g/mol}$
$32.0\text{ g/mol}$
$128.0\text{ g/mol}$
Step-by-step solution:
1. By Graham's law of effusion, the effusion rate $r$ of a gas through a small pinhole at constant $(P, T)$ is inversely proportional to the square root of its molar mass:
$$\frac{r_{\text{He}}}{r_{\text{unknown}}} = \sqrt{\frac{M_{\text{unknown}}}{M_{\text{He}}}}$$
2. Given $\frac{r_{\text{He}}}{r_{\text{unknown}}} = 4.0$ and $M_{\text{He}} = 4.0\text{ g/mol}$:
$$4.0 = \sqrt{\frac{M_{\text{unknown}}}{4.0}}$$
3. Squaring both sides:
$$16.0 = \frac{M_{\text{unknown}}}{4.0} \implies M_{\text{unknown}} = 16.0 \times 4.0 = 64.0\text{ g/mol}$$
चरण-दर-चरण समाधान:
1. ग्राहम के प्रवाह के नियम के अनुसार, स्थिर $(P, T)$ पर एक छोटे पिनहोल के माध्यम से गैस की प्रवाह दर $r$ उसके दाढ़ द्रव्यमान के वर्गमूल के व्युत्क्रमानुपाती होती है:
$$\frac{r_{\text{He}}}{r_{\text{unknown}}} = \sqrt{\frac{M_{\text{unknown}}}{M_{\text{He}}}}$$
2। दिया गया है $\frac{r_{\text{He}}}{r_{\text{unknown}}} = 4.0$ और $M_{\text{He}} = 4.0\text{ g/mol}$:
$$4.0 = \sqrt{\frac{M_{\text{unknown}}}{4.0}}$$
3. दोनों पक्षों का वर्ग करने पर:
$$16.0 = \frac{M_{\text{unknown}}}{4.0} \implies M_{\text{unknown}} = 16.0 \times 4.0 = 64.0\text{ g/mol}$$
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